3.1 Characterization of RE-M-GO composite
The SEM images of GO, LaCl3-M-GO-1, and LaCl3-M-GO-2 are shown in Fig. 1 (d), (e), and (f), are magnified views of the above-mentioned three cases, respectively. Fig. 1 (g) and (h) are magnified views of 240000 times that of LaCl3-M-GO-1, LaCl3-M-GO-2. Compared to the graphs (a), (b), (c), (d), (e), and (f), the agglomeration of graphene oxide with modification is significantly reduced. We can also observe the modified graphene oxide obtained by the heating method has better dispersibility than the infiltration. It can be seen that there are a lot of wrinkles on the surface of the modified graphene oxide from the high magnification of graphs (g) and (h). Earlier studies [20] have found that that the presence of a large number of wrinkles can improve the electrochemical properties of graphene compared to a flat graphene layer and it can increase the electrochemical current density as the battery electrode. The EDS showed that the La element has already been presented in the graphene oxide (Fig. 2).
Figure 3 (a) and (b) presents the CeCl3-M-GO-3 at a magnification of 1600 times and a magnification of 50,000 times. The same SEM magnification graphs of CeCl3-M-GO-4 are present in Figure 3 (c) and (d). It can be seen that the surface of the graphene oxide distributes a large number of particles. Combined with the energy spectrum (Fig. 4), it was determined that the particles are Ce. In addition, the modified graphene oxide is obtained by the heating modifier method exhibited a better dispersibility contrasted to infiltration.
To further confirm the structure of modified GO, XRD was used for phase identification, and the size of the rare earth oxide was calculated by the Debye-Scherr formula. The graphene oxide displayed a characteristic peak at 2θ = 11 °, with a d value of 8.81 angstroms. As shown in Fig. 5, the characteristic diffraction peaks of 2θ = 11 ° in the other three disappeared in contrast to LaCl3-M-GO-1, while LaCl3-M-GO-1 weakened a lot at 11° without disappearing completely. The diffraction peaks of graphene were observed at about 2θ = 23 ° in LaCl3-M-GO-1 and LaCl3-M-GO-2 indicating that the graphene lamellar spacing changed and the graphene oxide was partially reduced in the modification. Further, La2O3 appeared after modification, and its grain size is about 16 nm. However, CeCl3-M-GO-3 and CeCl3 -M-GO-4 only revealed the diffraction peaks of CeO2, and their grain sizes are about 16 and 14 nm. Combined with rare-earth compound particles appearing in the results of SEM, the main reason for the disappearance of characteristic diffraction peaks of GO can be attributed to the destruction of the regular layer of GO due to crystal growth of CeO2 between the intermediate layers of GO. The good crystallinity of CeO2 providing strong reflection coverage of the GO signal is another reason.
TEM images of GO, LaCl3-M-GO-1, CeCl3-M-GO-3 and CeCl3-M-GO-4 are shown in Fig. 6. A small number of particles appeared in graphene oxide in Fig. 6(b), which explains the reason why the graphene oxide diffraction peak of LaCl3-M-GO-1 in Fig. 5 did not completely disappear. Combined with the above EDS (Fig. 2) and XRD (Fig. 5), it is certain that the particles were lanthanum oxide. As presented in Fig. 6 (c), the surface of modified graphene oxide was densely covered with the aggregates of CeO2 nanoparticles comparing with GO (Fig. 6(a)). The dispersion of CeCl3-M-GO-4 was relatively not so dense but more uniform. The size of the nanoparticle in CeCl3-M-GO-3 was around 18 nm, while 16 nm in CeCl3-M-GO-4.the particle produced by the heating method is smaller aggregates than that of infiltration. These findings demonstrate that the modification effect of Ce is more obvious than La.
XPS studied the chemical state of the surface elements and reveals whether RE is grafted onto the surface of the graphene oxide. Considering the electron binding energy of C1s 284.6eV as an internal standard, the elemental content of the surface of the M-GO and GO was determined as shown in Table 2. Meanwhile, Table 2 also summarized the changes of the percentage of C and O elemental content in GO, CeCl3-M-GO-3 and CeCl3-M-GO-4. Compared with the GO, the content of the C element in CeCl3-M-GO-3 and CeCl3-M-GO-4 were decreased and oxygen was increased. Moreover, the change in the content of C and O elements prepared by the infiltration is larger than that of the heating method. Due to the low content of La oxide in LaCl3-M-GO, the signal-noise ratio of the XPS test was poor and the La spectrum was not obvious. Fig. 7 (a) is the survey of CeCl3-M-GO-3 spectrum. It can be seen from the figure that the surface of modified graphene oxide contains Ce elements, which is consistent with the previous SEM, TEM, and XRD findings. The binding energy of the trivalent cerium ions of CeCl3 in Fig. 7 (b) are 606.32 eV, 601.63 eV, 587.63 eV, and 583.27 eV, respectively. When Ce and O form oxides, both Ce3d3/2 and Ce3d5/2 produced shake-up peaks. Therefore, the etravalent Ce3d in CeCl3-M-GO-3(Fig. 7 (C) has an absorption peak at 912.02 eV, 908.42 eV, 901.54 eV, 898.99 eV, 889.44 eV and 882.95 eV, respectively. Comparing with the binding energy of CeCl3 in Fig. 7 (b), it is indicated that Ce has been successfully added to the surface of graphene oxide[21]. Therefore, the Ce3d in Ce-M-GO-3 produced a chemical shift, indicating the formation of Re-O complexes[22]. Fig. 7.(d) is a sub-peak fitting of the oxygen element of GO, from which it can be seen that the combination of oxygen contains O = C-O, C-O, C-O-C, -OH. Fig. 7 (e) and (f) is a sub-peak fitting of the oxygen elements of CeCl3-M-GO-3 and CeCl3-M-GO-4. Compared with the oxygen element of GO (Fig. 7 (d) and combined with Table.3, it can be seen that the binding energy of O = C-O, C-O, C-O-C, -OH in CeCl3-M-GO-3and CeCl3-M-GO-4 all moved toward the low potential field, indicating that the oxygen element in the coordination process to get electrons[23].
Table.2 Percentage of elemental content in graphene oxide
|
Elementary composition/%
|
Atom ratio
|
C1s
|
O1s
|
Ce3d
|
O/C
|
GO
|
95.4
|
4.6
|
------
|
0.048
|
M-GO-3
|
74.95
|
19.85
|
5.2
|
0.264
|
M-GO-4
|
91.4
|
8.05
|
0.55
|
0.088
|
Table.3 The form and content of oxygen in the graphene oxide
|
O1S
|
Energy(eV)
|
Percentage composition(%)
|
GO
|
C-O-C,-OH
|
531.03
|
39.06
|
O=C-O
|
533.46
|
42.32
|
C-O
|
534.64
|
18.62
|
CeCl3-M-GO-3
|
C-O-C,-OH
|
529
|
46.05
|
O=C-O
|
530.98
|
40.52
|
C-O
|
532.76
|
13.44
|
CeCl3-M-GO-4
|
C-O-C,-OH
|
529.09
|
35.56
|
O=C-O
|
530.70
|
50.39
|
C-O
|
532.56
|
14.06
|
FTIR spectra of RE-M-GO composite are exposed in Fig. 8. GO shows a peak around 3442 cm-1 attributed to –OH vibration. This part of the peak is mainly from the adsorption of water molecules, The peak near 1749 cm−1 corresponds to the C = O double-built stretching vibration in the carboxyl group and the absorption peak at 1615 cm−1 is assigned to -C=C-. The peak near 1380 cm−1 corresponds to the C-O-C stretching vibration region and 1176 cm−1 belongs to the C-OH bending absorption vibration peak in the GO structure [24]. From the infrared spectra, it can be shown that the structures of graphene oxide contain -OH, C-O-C, and C = O. From the figure, we can see the peak of 1380 cm-1 corresponding to C-O-C was enhanced after modification, 1749 cm−1,1615 cm-1 and 1176 cm−1 were weakened and red-shifted in the Vicinity of LaCl3-M-GO-1 andLaCl3-M-GO-2. However, all these peaks in CeCl3-M-GO-3 and CeCl3-M-GO-4 disappeared and shifted to a red shift. At the same time, a new peak appeared at 557 cm−1, which belongs to C-O-Ce [25]. while no new peak appeared at LaCl3-M-Go, indicating that the modification effect of La was not obvious. Surface functional groups of GO sheets can interact with RE elements causing reduced intensities and even disappearance of characteristic bands. However, the attachment of RE to GO seems to prevent the out-of-plane oscillations of functional groups [26].